J/A+A/636/A12   1.4≤z≤5.0 QSOs luminosity function  (Retana-Montenegro+, 2020)

The optical luminosity function of LOFAR radio-selected quasars at 1.4 ≤ z ≤ 5.0 in the NDWFS-Bootes field. Retana-Montenegro E., Roettgering H.J.A. <Astron. Astrophys. 636, A12 (2020)> =2020A&A...636A..12R 2020A&A...636A..12R (SIMBAD/NED BibCode)
ADC_Keywords: QSOs ; Redshifts Keywords: quasars: general - quasars: supermassive black holes - radio continuum: galaxies - galaxies: high-redshift Abstract: We present an estimate of the optical luminosity function (OLF) of LOFAR radio-selected quasars (RSQs) at 1.4<z<5.0 in the 9.3deg2 NOAO Deep Wide-field survey (NDWFS) of the Bootes field. The selection was based on optical and mid-infrared photometry used to train three different machine learning (ML) algorithms (Random forest, SVM, Bootstrap aggregation). Objects taken as quasars by the ML algorithms are required to be detected at ≥5σ significance in deep radio maps to be classified as candidate quasars. The optical imaging came from the Sloan Digital Sky Survey and the Pan-STARRS1 3{PI} survey; mid-infrared photometry was taken from the Spitzer Deep, Wide-Field Survey; and radio data was obtained from deep LOFAR imaging of the NDWFS-Bootes field. The requirement of a 5σ LOFAR detection allowed us to reduce the stellar contamination in our sample by two orders of magnitude. The sample comprises 130 objects, including both photometrically selected candidate quasars (47) and spectroscopically confirmed quasars (83). The spectral energy distributions calculated using deep photometry available for the NDWFS-Bootes field confirm the validity of the photometrically selected quasars using the ML algorithms as robust candidate quasars. The depth of our LOFAR observations allowed us to detect the radio-emission of quasars that would be otherwise classified as radio-quiet. Around 65% of the quasars in the sample are fainter than M1450=-24.0, a regime where the OLF of quasars selected through their radio emission, has not been investigated in detail. It has been demonstrated that in cases where mid-infrared wedge-based AGN selection is not possible due to a lack of appropriate data, the selection of quasars using ML algorithms trained with optical and infrared photometry in combination with LOFAR data provides an excellent approach for obtaining samples of quasars. The OLF of RSQs can be described by pure luminosity evolution at z<2.4, and a combined luminosity and density evolution at z>2.4. The faint-end slope, α, becomes steeper with increasing redshift. This trend is consistent with previous studies of faint quasars (M1450≤-22.0). We demonstrate that RSQs show an evolution that is very similar to that exhibited by faint quasars. By comparing the spatial density of RSQs with that of the total (radio-detected plus radio-undetected) faint quasar population at similar redshifts, we find that RSQs may compose up to ∼20% of the whole faint quasar population. This fraction, within uncertainties, is constant with redshift. Finally, we discuss how the compactness of the RSQs radio-morphologies and their steep spectral indices could provide valuable insights into how quasar and radio activity are triggered in these systems. Description: The catalog of spectroscopic and photometric presented here are used to calculate the optical luminosity function of radio-selected quasars in the NDWFS-Bootes field. File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file photom.dat 69 47 Photometric catalog spectros.dat 69 83 Spectroscopic catalog -------------------------------------------------------------------------------- See also: J/ApJS/161/9 : X-ray survey of the NDWFS Bootes field (Kenter+, 2005) J/ApJ/641/140 : Optical counterparts in the NDWFS Bootes field (Brand+, 2006) J/ApJ/772/26 : AGN with WISE. II. The NDWFS Bootes field (Assef+, 2013) Byte-by-byte Description of file: photom.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 19 A19 --- Source Source name (JHHMMSS.ss+DDMMSS.s) 21- 29 F9.5 deg RAdeg Right ascension (J2000) 31- 38 F8.5 deg DEdeg Declination (J2000) 40- 43 F4.2 --- zph Photometric redshift 45- 49 F5.2 mag imagPS Pan-Starrs i-band magnitude (AB) 51- 56 F6.2 mag 1450MAG Absolute magnitude at 1450Å 58- 63 F6.2 mJy F150MHz 150MHz LOFAR total flux density 65- 69 F5.2 mJy e_F150MHz rms uncertainty on F150MHz -------------------------------------------------------------------------------- Byte-by-byte Description of file: spectros.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 19 A19 --- Source Source name (JHHMMSS.ss+DDMMSS.s) 21- 29 F9.5 deg RAdeg Right ascension (J2000) 31- 38 F8.5 deg DEdeg Declination (J2000) 40- 43 F4.2 --- zsp Spectroscopic redshift 45- 49 F5.2 mag imagPS Pan-Starrs i-band magnitude (AB) 51- 56 F6.2 mag 1450MAG Absolute magnitude at 1450Å 58- 63 F6.2 mJy F150MHz 150MHz LOFAR total flux density 65- 69 F5.2 mJy e_F150MHz rms uncertainty on F150MHz -------------------------------------------------------------------------------- Acknowledgements: Edwin Retana-Montenegro, edwinretana(at)gmail.com
(End) Patricia Vannier [CDS] 03-Feb-2020
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